Camera lens

ABSTRACT

A camera lens is disclosed. The camera lens includes a first lens with positive refractive power; a second lens with negative refractive power; a third lens with negative refractive power; a fourth lens with positive refractive power; a fifth lens with negative refractive power; and a sixth lens with negative refractive power. The camera lens further satisfies specific conditions.

TECHNICAL FIELD

The present disclosure relates to the technical field of opticalelements, and more particularly to a camera lens used in a portabledevice.

RELATED ART OF THE PRESENT DISCLOSURE

The present invention relates to a camera lens. Particularly it relatesto a camera lens very suitable for mobile phone camera module and WEBcamera lens etc. equipped with high-pixel camera elements such as CCD,CMOS etc. The camera lens of the invention is composed of six piecetotal angle of view, narrow angle below 50°, and small sized lens withexcellent optical properties.

In recent years, various camera devices equipped with camera elementssuch as CCD, CMOS are extensively popular. Along with development oncamera lens toward miniaturization and high performance, narrow angleand small sized camera lenses with excellent optical properties areneeded in society.

The technology related to the camera lens composed of six piece smallsized lenses with excellent optical properties is developed gradually.The camera lens mentioned in the proposal is composed of six piecelenses which are arranged sequentially from object side as follows: afirst lens with positive refractive power; a second lens with negativerefractive power; a third lens with negative refractive power; a fourthlens with positive refractive power and a fifth lens with negativerefractive power; a sixth lens with negative refractive power

The camera lens disclosed in embodiment 1 of the prior Japanese PatentPublication No. 2015-175876 is composed of the above mentioned six piecelenses, but refractive power distribution of the first lens isinsufficient and shape of the fourth lens is improper; 2ω=83.4° so it iswide angle.

The camera lens disclosed in embodiment 6 of the prior Japanese PatentPublication No. 2015-121730 is composed of the above mentioned six piecelenses, but refractive power distribution of the first lens isinsufficient and shape of the fourth lens is improper; 2ω=74.0° so it iswide angle.

Therefore, it is necessary to provide an improved camera lens toovercome the disadvantages mentioned above.

BRIEF DESCRIPTION OF THE DRAWINGS

The present invention will hereinafter be described in detail withreference to exemplary embodiments. To make the technical problems to besolved, technical solutions and beneficial effects of present disclosuremore apparent, the present disclosure is described in further detailtogether with the figures and the embodiments. It should be understoodthe specific embodiments described hereby are only to explain thisdisclosure, not intended to limit this disclosure.

FIG. 1 is a structure diagram of a camera lens LA related to oneembodiment of the present disclosure.

FIG. 2 is a structure diagram of the definite Embodiment 1 of theabove-mentioned camera lens LA.

FIG. 3 is a spherical aberration diagram of the camera lens LA inEmbodiment 1.

FIG. 4 is a magnification chromatic aberration diagram of the cameralens LA in Embodiment 1.

FIG. 5 is an image surface curving diagram and distortion aberrationdiagram of the camera lens LA in Embodiment 1.

FIG. 6 is a structure diagram of the definite Embodiment 2 of theabove-mentioned camera lens LA.

FIG. 7 is spherical aberration diagram of the camera lens LA inEmbodiment 2.

FIG. 8 is a magnification chromatic aberration diagram of the cameralens LA in Embodiment 2.

FIG. 9 is an image surface curving diagram and distortion aberrationdiagram of the camera lens LA in Embodiment 2.

DETAILED DESCRIPTION OF EXEMPLARY EMBODIMENTS

The present invention will hereinafter be described in detail withreference to exemplary embodiments. To make the technical problems to besolved, technical solutions and beneficial effects of present disclosuremore apparent, the present disclosure is described in further detailtogether with the figures and the embodiments. It should be understoodthe specific embodiments described hereby are only to explain thisdisclosure, not intended to limit this disclosure.

FIG. 1 is the structure diagram of a camera lens LA related to one modeof execution in the invention. The camera lens LA is composed of sixpiece lenses which are arranged sequentially from the object side to theimaging surface including a first lens L1, a second lens L2, a thirdlens L3, a fourth lens L4, a fifth lens L5 and a sixth lens L6. A glassplate GF is arranged between the sixth lens L6 and the imaging surface.And a glass cover or an optical filter having the function of filteringIR can be taken as the glass plate GF. Moreover, it shall be fine if noglass plate GF is arranged between the sixth lens L6 and the imagingsurface.

The first lens L1 has positive refractive power; the second lens L2 hasnegative refractive power; the third lens L3 has negative refractivepower; the fourth lens L4 has positive refractive power; the fifth lensL5 has negative refractive power, the sixth lens has negative refractivepower. Moreover, the surfaces of the six piece lenses should be designedas the aspheric shape preferably in order to correct the aberrationwell.

A camera lens is characterized in that the camera lens meets followingconditions (1)˜(2):0.35≤f1/f≤0.50  (1)0.15≤d10/f≤0.25  (2)where,f: overall focal distance of the camera lensf1: focal distance of the first lensd10: axial distance from image side surface of the fifth lens L5 toobject side surface of the sixth lens L6

The positive refractive power of the first lens L1 is specified in thecondition (1). It is useful for development of small sized trend whenthe numerical range exceeds the lower limit specified in the condition(1); however, the aberration cannot be corrected easily because thepositive refractive power of the first lens L1 becomes too strong; onthe contrary, when the numerical range exceeds the upper limitspecified, the development of small sized trend cannot be implementedeasily because the refractive power of the first lens L1 becomes tooweak.

Therefore, numerical range of condition (1) should be set within thenumerical range of the following condition (1-A) preferably,0.42≤f1/f≤0.46  (1-A)

Ratio of axial distance from the image side surface of the fifth lens tothe object side surface of the sixth lens to overall focal distance ofthe camera lens is specified in condition (2). When it is outside therange of condition (2), 2ω≤50° incident angle of main light towardimaging surface (hereinafter referred to as CRA) cannot increase easily.Therefore, numerical range of condition (2) should be set within thenumerical range of the following condition (2-A) preferably,0.15≤d10/f≤0.20  (2-A)

The second lens L2 has negative refractive power and meets the followingcondition (3).−1.00≤f2/f≤−0.50  (3)where,f: overall focal distance of the camera lensf2: focal distance of the second lens

Negative refractive power of the second lens L2 is specified in thecondition (3). When it is outside the range of condition (3), 2ω≤50°,correction of chromatic aberration on axle and outside axle cannot beimplemented easily.

Therefore, numerical range of condition (3) should be set within thenumerical range of the following condition (3-A) preferably,−0.80≤f2/f≤−0.60  (3-A)

The third lens L3 has negative refractive power and meets the followingcondition (4).−10.00≤f3/f≤−2.00  (4)where,f: overall focal distance of the camera lensf3: focal distance of the third lens

The negative refractive power of the third lens L3 is specified in thecondition (4). When it is outside the range of condition (4), 2ω≤50°,correction of chromatic aberration outside axle cannot be implementedeasily.

Therefore, numerical range of condition (4) should be set within thenumerical range of the following condition (4-A) preferably,−8.00≤f3/f≤−3.00  (4-A)

The first lens L1 has positive refractive power and meets the followingcondition (5).−1.00≤(R1+R2)/(R1−R2)≤−0.80  (5)where,R1: curvature radius of the first lens' object side surfaceR2: curvature radius of the first lens' image side surface

The shape of the first lens L1 is specified in the condition (5). Whenit is outside the range of condition (5), 2ω≤50°, development of smallsized trend cannot be implemented easily.

Therefore, numerical range of condition (5) should be set within thenumerical range of the following condition (5-A) preferably,−0.95≤(R1+R2)/(R1−R2)≤−0.88  (5-A)

The sixth lens L6 has negative refractive power and meets the followingcondition (6).−4.00≤(R11+R12)/(R11−R12)≤−1.00  (6)where,R11: curvature radius of the sixth lens' object side surfaceR12: curvature radius of the sixth lens' image side surface

The shape of the sixth lens L6 is specified in the condition (6). Whenit is outside the range of condition (6), 2ω≤50° incident angle of mainlight toward imaging surface (hereinafter referred to as CRA) cannotincrease easily.

Therefore, numerical range of condition (6) should be set within thenumerical range of the following condition (6-A) preferably,−3.20≤(R11+R12)/(R11−R12)≤−2.00  (6-A)

Because six piece lenses of camera Lens LA all have the stated formationand meet all the conditions, so it is possible to produce a small sizedand 2ω≤50° narrow angle camera lens with excellent optical properties.

The camera lens LA of the invention shall be explained below by usingthe embodiments. Moreover, the symbols used in all embodiments are shownas follows. And mm shall be taken as the unit of the distance, theradius and the center thickness.

f: overall focal distance of the camera lens LA

f1: focal distance of the first lens L1

f2: focal distance of the second lens L2

f3: focal distance of the third lens L3

f4: focal distance of the fourth lens L4

f5: focal distance of the fifth lens L5

f6: focal distance of the sixth lens L6

Fno: F Value

2ω: total angle of view

CRA: incident angle of main light toward imaging surface

S1: Open aperture

R: curvature radius of optical surface, if a lens is involved it iscentral curvature radius

R1: curvature radius of the first lens L1's object side surface

R2: curvature radius of the first lens L1's image side surface

R3: curvature radius of the second lens L2's object side surface

R4: curvature radius of the second lens L2's image side surface

R5: curvature radius of the third lens L3's object side surface

R6: curvature radius of the third lens L3's image side surface

R7: curvature radius of the fourth lens L4's object side surface

R8: curvature radius of the fourth lens L4's image side surface

R9: curvature radius of the fifth lens L5's object side surface

R10: curvature radius of the fifth lens L5's image side surface

R11: curvature radius of the sixth lens L6's object side surface

R12: curvature radius of the sixth lens L6's image side surface

R13: curvature radius of the glass plate GF's object side surface

R14: curvature radius of the glass plate GF's image side surface

d: center thickness of lenses or the distance between lenses

d0: axial distance from open aperture S1 to object side surface of thefirst lens L1

d1: center thickness of the first lens L1

d2: axial distance from image side surface of the first lens L1 toobject side surface of the second lens L2

d3: center thickness of the second lens L2

d4: axial distance from image side surface of the second lens L2 toobject side surface of the third lens L3

d5: center thickness of the third lens L3

d6: axial distance from image side surface of the third lens L3 toobject side surface of the fourth lens L4

d7: center thickness of the fourth lens L4

d8: axial distance from image side surface of the fourth lens L4 toobject side surface of the fifth lens L5

d9: center thickness of the fifth lens L5

d10: axial distance from image side surface of the fifth lens L5 toobject side surface of the sixth lens L6

d11: center thickness of the sixth lens L6

d12: axial distance from image side surface of the sixth lens L6 toobject side surface of the glass plate GF

d13: center thickness of glass plate GF

d14: axial distance from image side surface to imaging surface of theglass plate GF

nd: refractive power of line d

nd1: refractive power the first lens L1's line d

nd2: refractive power the second lens L2's line d

nd3: refractive power the third lens L3's line d

nd4: refractive power the fourth lens L4's line d

nd5: refractive power the fifth lens L5's line d

nd6: refractive power the sixth lens L6's line d

nd7: refractive power the glass plate GF's line d

νd: abbe number

ν1: abbe number of the first lens L1

ν2: abbe number of the second lens L2

ν3: abbe number of the third lens L3

ν4: abbe number of the fourth lens L4

ν5: abbe number of the fifth lens L5

ν6: abbe number of the sixth lens L6

ν6: abbe number of the glass plate GF

TTL: optical length (axial distance from object side surface to theimaging surface of the first lens L1)

LB: axial distance (including thickness of the glass plate GF) from theimage side surface to the imaging surface of the sixth lens L6;y=(x2/R)/[1+{1−(k+1)(x2/R2)}½]+A4x4+A6x6+A8x8+A10x10+A12x12+A14x14+A16x16  (7)where, R is axial curvature radius, k is cone coefficient, A4, A6, A8,A10, A12, A14, A16 are aspheric coefficients.

For convenience sake, the aspheric surface shown in the formula (7)shall be taken as the aspheric surfaces of all lens' surfaces. However,the invention shall not be limited to polynomial form of the asphericsurface shown in the formula (7).

Embodiment 1

FIG. 2 is the structure of camera lens LA in Embodiment 1. Data shown inTable 1: curvature radius R of the object side surfaces and the imageside surfaces, center thicknesses of the lenses, distances d among thelenses, refractive powers nd and abbe numbers of the lens L1˜L6 in theEmbodiment 1, wherein the camera lens LA is formed by the lens L1˜L6;Data shown in Table 2: conical coefficients k and aspheric coefficients

TABLE 1 R d nd vd S1 ∞ d0 = −0.450 R1 1.46653 d1 = 0.807 nd1 1.5441 v156.12 R2 −36.23577 d2 = 0.112 R3 −13.20291 d3 = 0.252 nd2 1.6614 v220.41 R4 3.27080 d4 = 0.376 R5 11.24906 d5 = 0.260 nd3 1.5441 v3 56.12R6 6.05696 d6 = 0.068 R7 8.99571 d7 = 0.271 nd4 1.6614 v4 20.41 R8−16.84601 d8 = 0.540 R9 −2.87062 d9 = 0.274 nd5 1.5441 v5 56.12 R10−7.30957 d10 = 1.029 R11 −3.43403 d11 = 0.532 nd6 1.5441 v6 56.12 R12−8.01817 d12 = 0.480 R13 ∞ d13 = 0.210 nd7 1.5168 v7 64.17 R14 ∞ d14 =0.169

TABLE 2 conical coefficient aspheric coefficient k A4 A6 A8 A10 A12 A14A16 R1 3.8797E−02 −8.6349E−03 1.8872E−02 −3.1907E−02 2.4884E−02−5.1492E−03 −2.5306E−03 2.3164E−03 R2 0.0000E+00 1.4395E−02 2.0032E−034.1725E−02 −2.1366E−02 4.5550E−03 2.8987E−04 −6.8014E−03 R3 0.0000E+004.4815E−02 2.3098E−02 2.0637E−02 −2.1764E−03 −2.0084E−02 −2.8682E−021.3827E−02 R4 1.0616E+01 3.3679E−02 4.4085E−02 2.0240E−02 −7.4655E−02−1.4336E−02 5.9695E−02 −8.9665E−02 R5 0.0000E+00 1.8504E−03 −2.0517E−02−7.4434E−03 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 R6 0.0000E+00−4.5186E−03 −1.8754E−02 −5.9149E−02 0.0000E+00 0.0000E+00 0.0000E+000.0000E+00 R7 0.0000E+00 −2.9244E−02 2.0252E−02 −1.7633E−02 −1.8032E−02−3.2755E−02 5.0924E−03 2.6892E−02 R8 −3.7089E+02 −6.0421E−02 1.8380E−02−1.4875E−03 6.1141E−02 −2.7073E−02 −1.9848E−01 1.7189E−01 R9 2.8150E+00−1.5703E−01 −7.1453E−03 −1.5679E−02 −1.3447E−02 −3.6254E−03 −6.0916E−027.1271E−02 R10 1.1305E+01 −6.3317E−02 3.4117E−02 −2.3385E−02 7.3229E−032.3969E−03 1.4991E−03 −1.0770E−03 R11 0.0000E+00 1.6235E−05 7.0843E−03−1.3120E−03 −5.8744E−04 1.0556E−04 5.2411E−05 −9.4666E−06 R12 1.3121E+00−2.7254E−02 4.6027E−03 −1.8396E−03 4.1932E−04 −4.1434E−05 −1.6463E−053.7041E−06

The values in embodiment 1 and 2 and the values corresponding to theparameters specified in the conditions (1)˜(6) are shown in subsequentTable 5.

As shown on Table 5, the Embodiment 1 meets the conditions (1)˜(6).

Spherical aberration of camera lens LA in embodiment 1 is shown in FIG.3, magnification chromatic aberration of the same is shown in FIG. 4,image surface curving and distortion aberration of the same is shown inFIG. 5. Furthermore, image surface curving S in FIG. 5 is the oneopposite to the sagittal image surface, T is the one opposite to thetangent image surface. Same applies for the Embodiment 2. As shown inFIG. 3˜5, the camera lens LA in embodiment 1 has the properties asfollows: 2ω=47.5°, TTL=5.380 mm, camera lens is small sized and narrowangle camera lens, it is not difficult to understand why it hasexcellent optical properties.

Embodiment 2

FIG. 6 is the structure of camera lens LA in Embodiment 2. Data shown inTable 3: curvature radius R of the object side surfaces and the imageside surfaces, center thicknesses of the lenses, distances d among thelenses, refractive powers nd and abbe numbers of the lens L1˜L6 in theEmbodiment 2, wherein the camera lens LA is formed by the lens L1˜L6;Data shown in Table 4: conical coefficients k and aspheric coefficients

TABLE 3 R d nd vd S1 ∞ d0 = −0.450 R1 1.46974 d1 = 0.810 nd1 1.5441 v156.12 R2 −34.31642 d2 = 0.114 R3 −13.21482 d3 = 0.253 nd2 1.6614 v220.41 R4 3.27387 d4 = 0.373 R5 10.92318 d5 = 0.264 nd3 1.5441 v3 56.12R6 5.96396 d6 = 0.065 R7 8.96335 d7 = 0.273 nd4 1.6510 v4 21.51 R8−16.91035 d8 = 0.540 R9 −2.87313 d9 = 0.272 nd5 1.5441 v5 56.12 R10−7.33145 d10 = 1.031 R11 −3.45705 d11 = 0.519 nd6 1.5441 v6 56.12 R12−8.13963 d12 = 0.480 R13 ∞ d13 = 0.210 nd7 1.5168 v7 64.17 R14 ∞ d14 =0.169

TABLE 4 conical coefficient aspheric coefficient k A4 A6 A8 A10 A12 A14A16 R1 3.6206E−02 −7.8902E−03 1.7961E−02 −3.1925E−02 2.4935E−02−5.1548E−03 −2.5779E−03 2.2510E−03 R2 0.0000E+00 1.3927E−02 1.7007E−034.1313E−02 −2.1565E−02 4.5652E−03 4.3408E−04 −6.5933E−03 R3 0.0000E+004.5219E−02 2.3590E−02 2.1427E−02 −1.6792E−03 −1.9994E−02 −2.8926E−021.3373E−02 R4 1.0568E+01 3.4016E−02 4.7020E−02 1.7544E−02 −7.7987E−02−1.4696E−02 6.4300E−02 −8.0303E−02 R5 0.0000E+00 1.6427E−03 −2.3412E−02−8.8777E−03 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 R6 0.0000E+00−4.0791E−03 −1.6708E−02 −6.0612E−02 0.0000E+00 0.0000E+00 0.0000E+000.0000E+00 R7 0.0000E+00 −2.9686E−02 1.8846E−02 −1.6595E−02 −1.6710E−02−3.2703E−02 5.4007E−03 2.8267E−02 R8 −3.6688E+02 −6.0051E−02 1.8862E−02−2.7744E−03 5.8220E−02 −2.9022E−02 −1.9877E−01 1.7250E−01 R9 2.7424E+00−1.5645E−01 −6.1243E−03 −1.4799E−02 −1.2882E−02 −3.4769E−03 −6.1231E−027.0634E−02 R10 1.1639E+01 −6.3511E−02 3.4027E−02 −2.3423E−02 7.3218E−032.4192E−03 1.5429E−03 −1.0185E−03 R11 0.0000E+00 2.7978E−05 7.0849E−03−1.3121E−03 −5.8753E−04 1.0550E−04 5.2382E−05 −9.4802E−06 R12 1.3317E+00−2.7262E−02 4.6048E−03 −1.8392E−03 4.1940E−04 −4.1418E−05 −1.6459E−053.7052E−06

As shown on Table 5, the Embodiment 2 meets the conditions (1)˜(6).

Spherical aberration of camera lens LA in embodiment 2 is shown in FIG.7, magnification chromatic aberration of the same is shown in FIG. 8,image surface curving and distortion aberration of the same is shown inFIG. 9. As shown in FIG. 3˜5, the camera lens LA in embodiment 2 has theproperties as follows: 2ω=47.5°, TTL/IH=5.380 mm, camera lens is smallsized and narrow angle camera lens, it is not difficult to understandwhy it has excellent optical properties.

The values in all embodiments and the values corresponding to theparameters specified in the conditions (1)˜(6) are shown in the Table 5.Furthermore, units of various values in Table 5 are respectively 2ω(°),f(mm), f1 (mm), f2 (mm), f3 (mm), f4 (mm), f5 (mm), f6 (mm), TTL(mm),LB(mm), IH(mm).

TABLE 5 Embodiment 1 Embodiment 2 Condition f1/f 0.448 0.448 1 d10/f0.177 0.177 2 f2/f −0.676 −0.676 3 f3/f −4.214 −4.227 4 (R1 + R2)/(R1 −R2) −0.922 −0.918 5 (R11 + R12)/(R11 − R12) −2.498 −2.477 6 Fno 2.652.65 2ω 47.5 47.5 Max CRA 27.0 27.0 f 5.827 5.832 f1 2.610 2.611 f2−3.940 −3.943 f3 −24.553 −24.651 f4 8.904 9.038 f5 −8.881 −8.875 f6−11.510 −11.494 TTL 5.380 5.373 LB 0.859 0.859 IH 2.619 2.619

It is to be understood, however, that even though numerouscharacteristics and advantages of the present exemplary embodiments havebeen set forth in the foregoing description, together with details ofthe structures and functions of the embodiments, the disclosure isillustrative only, and changes may be made in detail, especially inmatters of shape, size, and arrangement of parts within the principlesof the invention to the full extent indicated by the broad generalmeaning of the terms where the appended claims are expressed.

What is claimed is:
 1. A camera lens comprising, arranged sequentiallyfrom an object side to an image side: a first lens with positiverefractive power; a second lens with negative refractive power; a thirdlens with negative refractive power; a fourth lens with positiverefractive power; a fifth lens with negative refractive power; and asixth lens with negative refractive power; wherein the camera lensfurther satisfies the following conditions (1)˜(2):0.35≤f1/f≤0.50  (1)0.15≤d10/f≤0.25  (2) where, f: overall focal distance of the cameralens; f1: focal distance of the first lens; d10: axial distance fromimage side surface of the fifth lens to object side surface of the sixthlens.
 2. The camera lens as described in claim 1 further satisfyingfollowing condition (3):−1.00≤f2/f≤−0.50  (3) where, f: overall focal distance of the cameralens; f2: focal distance of the second lens.
 3. The camera lens asdescribed in claim 1 further satisfying following condition (4):−10.00≤f3/f≤−2.00  (4) where, f: overall focal distance of the cameralens; f3: focal distance of the third lens.
 4. The camera lens asdescribed in claim 1 further satisfying following condition (5):−1.00≤(R1+R2)/(R1−R2)≤−0.80  (5) where, R1: curvature radius of thefirst lens' object side surface; R2: curvature radius of the first lens'image side surface.
 5. The camera lens as described in claim 1 furthersatisfying following condition (6):−4.00≤(R11+R12)/(R11−R12)≤−1.00  (1) where, R11: curvature radius of thesixth lens' object side surface; R12: curvature radius of the sixthlens' image side surface.